ENTRY F0199 20200627 F079F019900000001 SUBENT F0199001 20200627 F079F019900100001 BIB 9 23 F019900100002 TITLE (He3,d) and (He3,t) reactions on 9Be and 11B F019900100003 AUTHOR (M.A.Crosby,J.C.Legg) F019900100004 INSTITUTE (1USARIC) F019900100005 REFERENCE (J,NP/A,95,639,1967) F019900100006 FACILITY (VDG,1USARIC) F019900100007 METHOD (EDE,BCINT) F019900100008 DETECTOR (TELES,SI) dE/dx-E counter telescope. DeltaE was a thinF019900100009 (6mg/cm2) totally depleted silicon detector. F019900100010 E detector was a 3mm lithium drifted silicon detector. F019900100011 A detector placed in a port located at 30.degr. to the F019900100012 beam was used to monitor the elastically scattered ionsF019900100013 ERR-ANALYS (ERR-T) Absolute error F019900100014 (DATA-ERR) Error from graphic bars (relative errors). F019900100015 The relative errors were calculated from counting F019900100016 statistics and, in some cases, were increased to F019900100017 indicate uncertainty in particle identification. F019900100018 HISTORY (19841101C) F019900100019 (19990409U) CNPD: corrected 4-dig. year and lower casesF019900100020 (20071123A) Author's name was changed. Error F019900100021 designation (ANG-ERR-D) was changed. F019900100022 (20200627A) SD: Corrections in all Subents. BIB updatedF019900100023 The accuracy of data presentation has been revised. F019900100024 Author's name corrected (M.A.Grosby -> M.A.Crosby) F019900100025 ENDBIB 23 0 F019900100026 COMMON 2 3 F019900100027 EN ANG-ERR-D F019900100028 MEV ADEG F019900100029 10.0 1.2 F019900100030 ENDCOMMON 3 0 F019900100031 ENDSUBENT 30 0 F019900199999 SUBENT F0199002 20200627 F079F019900200001 BIB 4 6 F019900200002 REACTION (4-BE-9(HE3,T)5-B-9,PAR,DA) F019900200003 SAMPLE The target chamber was a 10 cm high circular brass F019900200004 cylinder with an inside diameter of 30 cm. F019900200005 STATUS (CURVE) fig 4 from Nucl.Phys.,A95(1967),639 F019900200006 HISTORY (20200627A) SD: SF9=EXP deleted from REACTION code. F019900200007 EN-SEC deleted. STATUS updated. SAMPLE added. F019900200008 ENDBIB 6 0 F019900200009 COMMON 1 3 F019900200010 ERR-T F019900200011 PER-CENT F019900200012 15. F019900200013 ENDCOMMON 3 0 F019900200014 DATA 4 29 F019900200015 E-LVL ANG-CM DATA-CM DATA-ERR F019900200016 MEV ADEG MB/SR MB/SR F019900200017 0. 12.8 0.888 0.189 F019900200018 0. 19.8 0.573 0.126 F019900200019 0. 26.9 0.352 0.084 F019900200020 0. 33.3 0.477 0.094 F019900200021 0. 40.7 0.582 0.136 F019900200022 0. 46.8 0.424 0.105 F019900200023 0. 54.1 0.392 0.094 F019900200024 0. 60.3 0.371 0.073 F019900200025 0. 66.6 0.381 0.094 F019900200026 0. 72.8 0.359 0.073 F019900200027 0. 78.0 0.359 0.052 F019900200028 0. 84.3 0.379 0.063 F019900200029 0. 90.5 0.316 0.042 F019900200030 0. 94.6 0.242 0.042 F019900200031 0. 99.9 0.357 0.052 F019900200032 0. 106.2 0.294 0.042 F019900200033 0. 111.4 0.314 0.031 F019900200034 0. 116.6 0.324 0.052 F019900200035 0. 120.8 0.387 0.052 F019900200036 0. 130.2 0.417 0.063 F019900200037 2.34 22.1 0.315 0.072 F019900200038 2.34 29.2 0.211 0.062 F019900200039 2.34 36.4 0.128 0.057 F019900200040 2.34 43.6 0.092 0.062 F019900200041 2.34 50.9 0.081 0.047 F019900200042 2.34 57.1 0.060 0.036 F019900200043 2.34 63.5 0.091 0.047 F019900200044 2.34 70.9 0.178 0.036 F019900200045 2.34 83.3 0.121 0.041 F019900200046 ENDDATA 31 0 F019900200047 ENDSUBENT 46 0 F019900299999 SUBENT F0199003 20200627 F079F019900300001 BIB 4 7 F019900300002 REACTION (5-B-11(HE3,T)6-C-11,PAR,DA) F019900300003 SAMPLE Enriched 11B target. The target chamber was a 10 cm F019900300004 high circular brass cylinder with an inside F019900300005 diam. of 30 cm. F019900300006 STATUS (CURVE) fig 5 from Nucl.Phys.,A95(1967),639 F019900300007 HISTORY (20200627A) SD: SF9=EXP deleted from REACTION code. F019900300008 EN-SEC deleted. STATUS updated. SAMPLE added. F019900300009 ENDBIB 7 0 F019900300010 COMMON 1 3 F019900300011 ERR-T F019900300012 PER-CENT F019900300013 30. F019900300014 ENDCOMMON 3 0 F019900300015 DATA 4 28 F019900300016 E-LVL ANG-CM DATA-CM DATA-ERR F019900300017 MEV ADEG MB/SR MB/SR F019900300018 0. 18.1 1.443 0.125 F019900300019 0. 25.3 1.549 0.146 F019900300020 0. 32.5 1.697 0.083 F019900300021 0. 37.9 1.469 0.083 F019900300022 0. 44.3 1.283 0.104 F019900300023 0. 51.8 1.014 0.083 F019900300024 0. 57.2 0.662 0.083 F019900300025 0. 63.5 0.642 0.063 F019900300026 0. 69.7 0.644 0.083 F019900300027 0. 82.1 0.835 0.083 F019900300028 0. 86.3 0.836 0.063 F019900300029 0. 103.1 0.674 0.063 F019900300030 0. 108.4 0.571 0.083 F019900300031 0. 116.8 0.449 0.104 F019900300032 0. 126.2 0.535 0.104 F019900300033 2. 20.8 0.404 0.062 F019900300034 2. 27.1 0.410 0.047 F019900300035 2. 34.6 0.307 0.021 F019900300036 2. 40.1 0.224 0.021 F019900300037 2. 47.4 0.204 0.026 F019900300038 2. 53.9 0.142 0.031 F019900300039 2. 60.2 0.106 0.021 F019900300040 2. 67.6 0.076 0.016 F019900300041 2. 73.9 0.076 0.021 F019900300042 2. 80.1 0.087 0.021 F019900300043 2. 86.3 0.087 0.021 F019900300044 2. 92.6 0.093 0.021 F019900300045 2. 97.7 0.135 0.016 F019900300046 ENDDATA 30 0 F019900300047 ENDSUBENT 46 0 F019900399999 SUBENT F0199004 20200627 F079F019900400001 BIB 4 6 F019900400002 REACTION (4-BE-9(HE3,D)5-B-10,PAR,DA) F019900400003 SAMPLE The target chamber was a 10 cm high circular brass F019900400004 cylinder with an inside diameter of 30 cm. F019900400005 STATUS (CURVE) fig 6,7,8,9,10 from Nucl.Phys.,A95(1967),639 F019900400006 HISTORY (20200627A) SD: SF9=EXP deleted from REACTION code. F019900400007 EN-SEC deleted. STATUS updated. SAMPLE added. F019900400008 ENDBIB 6 0 F019900400009 COMMON 1 3 F019900400010 ERR-T F019900400011 PER-CENT F019900400012 15. F019900400013 ENDCOMMON 3 0 F019900400014 DATA 4 170 F019900400015 E-LVL ANG-CM DATA-CM DATA-ERR F019900400016 MEV ADEG MB/SR MB/SR F019900400017 0. 12.1 8.436 0.812 F019900400018 0. 18.1 9.235 0.583 F019900400019 0. 24.5 6.435 0.580 F019900400020 0. 29.6 2.942 0.462 F019900400021 0. 35.1 1.421 0.059 F019900400022 0. 42.0 1.173 0.059 F019900400023 0. 49.1 1.622 0.059 F019900400024 0. 55.0 1.841 0.059 F019900400025 0. 60.8 1.480 0.059 F019900400026 0. 66.6 1.236 0.059 F019900400027 0. 72.3 0.759 0.059 F019900400028 0. 77.0 0.516 0.059 F019900400029 0. 82.9 0.736 0.059 F019900400030 0. 88.7 0.839 0.059 F019900400031 0. 94.6 0.826 0.059 F019900400032 0. 99.3 0.816 0.059 F019900400033 0. 103.9 0.806 0.059 F019900400034 0. 108.6 0.679 0.059 F019900400035 0. 113.3 0.669 0.059 F019900400036 0. 122.7 0.881 0.059 F019900400037 0. 127.3 0.754 0.059 F019900400038 0. 132.0 0.976 0.059 F019900400039 0. 136.7 0.966 0.059 F019900400040 0. 140.2 0.842 0.059 F019900400041 0. 143.7 1.066 0.059 F019900400042 0. 148.4 1.056 0.059 F019900400043 0. 151.9 0.933 0.059 F019900400044 0. 156.6 1.154 0.059 F019900400045 0. 160.1 1.147 0.059 F019900400046 0. 163.7 1.255 0.059 F019900400047 0.717 12.7 8.162 0.583 F019900400048 0.717 19.6 7.912 0.580 F019900400049 0.717 23.6 5.233 0.577 F019900400050 0.717 31.0 2.196 0.464 F019900400051 0.717 36.5 0.790 0.066 F019900400052 0.717 42.3 0.543 0.066 F019900400053 0.717 49.4 0.874 0.066 F019900400054 0.717 55.2 0.976 0.066 F019900400055 0.717 61.0 0.613 0.066 F019900400056 0.717 66.8 0.483 0.066 F019900400057 0.717 72.6 0.237 0.066 F019900400058 0.717 78.4 0.338 0.066 F019900400059 0.717 84.3 0.324 0.066 F019900400060 0.717 89.0 0.545 0.066 F019900400061 0.717 93.6 0.533 0.066 F019900400062 0.717 100.6 0.400 0.066 F019900400063 0.717 105.3 0.504 0.066 F019900400064 0.717 109.9 0.261 0.066 F019900400065 0.717 113.4 0.252 0.066 F019900400066 0.717 123.9 0.226 0.066 F019900400067 0.717 128.6 0.099 0.066 F019900400068 0.717 133.3 0.203 0.066 F019900400069 0.717 137.9 0.192 0.066 F019900400070 0.717 141.4 0.183 0.066 F019900400071 0.717 144.9 0.291 0.066 F019900400072 0.717 148.5 0.398 0.066 F019900400073 0.717 153.2 0.503 0.066 F019900400074 0.717 157.9 0.723 0.066 F019900400075 0.717 161.4 0.715 0.066 F019900400076 0.717 166.1 0.819 0.066 F019900400077 1.74 13.1 5.252 0.694 F019900400078 1.74 19.7 4.377 0.521 F019900400079 1.74 24.7 2.637 0.405 F019900400080 1.74 31.0 1.126 0.289 F019900400081 1.74 37.7 0.425 0.031 F019900400082 1.74 44.6 0.302 0.031 F019900400083 1.74 50.4 0.411 0.031 F019900400084 1.74 56.3 0.578 0.031 F019900400085 1.74 62.1 0.514 0.031 F019900400086 1.74 67.8 0.392 0.031 F019900400087 1.74 73.6 0.212 0.031 F019900400088 1.74 79.3 0.090 0.031 F019900400089 1.74 85.2 0.199 0.031 F019900400090 1.74 89.8 0.252 0.031 F019900400091 1.74 95.6 0.246 0.031 F019900400092 1.74 101.4 0.297 0.031 F019900400093 1.74 106.1 0.292 0.031 F019900400094 1.74 110.7 0.287 0.031 F019900400095 1.74 116.5 0.338 0.031 F019900400096 1.74 125.8 0.270 0.031 F019900400097 1.74 129.3 0.266 0.031 F019900400098 1.74 131.6 0.264 0.031 F019900400099 1.74 137.4 0.257 0.031 F019900400100 1.74 142.0 0.252 0.031 F019900400101 1.74 146.7 0.247 0.031 F019900400102 1.74 150.2 0.301 0.031 F019900400103 1.74 153.6 0.240 0.031 F019900400104 1.74 157.1 0.294 0.031 F019900400105 1.74 161.8 0.346 0.031 F019900400106 1.74 164.1 0.228 0.031 F019900400107 2.15 12.2 3.777 0.851 F019900400108 2.15 19.0 3.429 0.739 F019900400109 2.15 25.7 2.741 0.625 F019900400110 2.15 32.4 1.882 0.796 F019900400111 2.15 37.8 0.854 0.341 F019900400112 2.15 43.6 0.734 0.042 F019900400113 2.15 50.6 0.784 0.042 F019900400114 2.15 55.2 0.553 0.042 F019900400115 2.15 62.2 0.432 0.042 F019900400116 2.15 67.9 0.313 0.042 F019900400117 2.15 73.8 0.421 0.042 F019900400118 2.15 80.8 0.414 0.042 F019900400119 2.15 84.3 0.354 0.042 F019900400120 2.15 90.1 0.349 0.042 F019900400121 2.15 96.0 0.400 0.042 F019900400122 2.15 100.6 0.339 0.042 F019900400123 2.15 106.5 0.390 0.042 F019900400124 2.15 111.2 0.442 0.042 F019900400125 2.15 115.9 0.494 0.042 F019900400126 2.15 125.2 0.372 0.042 F019900400127 2.15 131.0 0.423 0.042 F019900400128 2.15 134.5 0.306 0.042 F019900400129 2.15 138.0 0.303 0.042 F019900400130 2.15 141.5 0.299 0.042 F019900400131 2.15 146.1 0.238 0.042 F019900400132 2.15 150.9 0.404 0.042 F019900400133 2.15 154.3 0.230 0.042 F019900400134 2.15 157.8 0.340 0.042 F019900400135 2.15 162.5 0.279 0.042 F019900400136 2.15 166.0 0.389 0.042 F019900400137 3.59 19.2 2.491 0.288 F019900400138 3.59 25.5 1.167 0.144 F019900400139 3.59 31.4 0.736 0.144 F019900400140 3.59 38.5 0.449 0.086 F019900400141 3.59 44.3 0.364 0.011 F019900400142 3.59 51.3 0.394 0.011 F019900400143 3.59 58.2 0.424 0.011 F019900400144 3.59 62.9 0.397 0.011 F019900400145 3.59 75.7 0.284 0.011 F019900400146 4.77 18.9 0.603 0.145 F019900400147 4.77 25.9 0.558 0.122 F019900400148 4.77 32.0 0.361 0.061 F019900400149 4.77 39.1 0.262 0.053 F019900400150 4.77 44.8 0.354 0.053 F019900400151 4.77 51.9 0.240 0.046 F019900400152 4.77 57.6 0.316 0.061 F019900400153 4.77 64.6 0.309 0.053 F019900400154 4.77 77.5 0.249 0.053 F019900400155 5.16 19.8 3.116 0.272 F019900400156 5.16 25.9 2.497 0.195 F019900400157 5.16 33.2 1.761 0.156 F019900400158 5.16 39.2 1.336 0.117 F019900400159 5.16 47.4 1.068 0.014 F019900400160 5.16 53.2 1.149 0.014 F019900400161 5.16 60.3 0.958 0.014 F019900400162 5.16 77.6 1.122 0.014 F019900400163 5.92 21.6 1.759 0.227 F019900400164 5.92 28.9 1.422 0.182 F019900400165 5.92 34.3 0.788 0.114 F019900400166 5.92 42.3 0.815 0.114 F019900400167 5.92 49.4 0.704 0.114 F019900400168 5.92 56.4 0.594 0.114 F019900400169 5.92 63.3 0.688 0.090 F019900400170 5.92 69.2 0.532 0.136 F019900400171 5.92 82.2 0.311 0.091 F019900400172 6.16 22.6 1.461 0.163 F019900400173 6.16 28.2 1.204 0.163 F019900400174 6.16 36.1 0.760 0.093 F019900400175 6.16 43.0 0.549 0.093 F019900400176 6.16 49.9 0.501 0.093 F019900400177 6.16 56.9 0.454 0.070 F019900400178 6.16 63.8 0.336 0.070 F019900400179 6.57 22.7 0.591 0.078 F019900400180 6.57 29.4 0.497 0.078 F019900400181 6.57 37.3 0.403 0.062 F019900400182 6.57 43.8 0.208 0.047 F019900400183 6.57 50.9 0.261 0.047 F019900400184 6.57 57.8 0.245 0.039 F019900400185 6.57 64.6 0.182 0.047 F019900400186 6.57 71.7 0.220 0.039 F019900400187 ENDDATA 172 0 F019900400188 ENDSUBENT 187 0 F019900499999 SUBENT F0199005 20200627 F079F019900500001 BIB 4 7 F019900500002 REACTION (5-B-11(HE3,D)6-C-12,PAR,DA) F019900500003 SAMPLE Enriched 11B target. The target chamber was a 10 cm F019900500004 high circular brass cylinder with an inside F019900500005 diam. of 30 cm. F019900500006 STATUS (CURVE) fig 11,12 from Nucl.Phys.,A95(1967),639 F019900500007 HISTORY (20200627A) SD: SF9=EXP deleted from REACTION code. F019900500008 EN-SEC deleted. STATUS updated. SAMPLE added. F019900500009 ENDBIB 7 0 F019900500010 COMMON 1 3 F019900500011 ERR-T F019900500012 PER-CENT F019900500013 30. F019900500014 ENDCOMMON 3 0 F019900500015 DATA 4 100 F019900500016 E-LVL ANG-CM DATA-CM DATA-ERR F019900500017 MEV ADEG MB/SR MB/SR F019900500018 0. 17.0 1.148 0.104 F019900500019 0. 22.0 0.792 0.083 F019900500020 0. 26.9 0.395 0.010 F019900500021 0. 33.1 0.268 0.010 F019900500022 0. 39.4 0.328 0.010 F019900500023 0. 45.7 0.347 0.010 F019900500024 0. 50.9 0.367 0.010 F019900500025 0. 55.0 0.324 0.010 F019900500026 0. 61.2 0.218 0.010 F019900500027 0. 66.4 0.195 0.010 F019900500028 0. 72.7 0.173 0.010 F019900500029 0. 77.9 0.150 0.010 F019900500030 0. 83.1 0.128 0.010 F019900500031 0. 88.3 0.126 0.010 F019900500032 0. 92.5 0.146 0.010 F019900500033 0. 97.7 0.123 0.010 F019900500034 0. 107.1 0.120 0.010 F019900500035 0. 116.5 0.097 0.010 F019900500036 0. 126.9 0.073 0.010 F019900500037 0. 136.4 0.112 0.063 F019900500038 0. 145.7 0.046 0.010 F019900500039 4.43 18.4 2.653 0.145 F019900500040 4.43 24.4 2.259 0.104 F019900500041 4.43 28.0 1.225 0.083 F019900500042 4.43 33.9 0.707 0.041 F019900500043 4.43 39.1 0.602 0.062 F019900500044 4.43 45.3 0.518 0.062 F019900500045 4.43 51.7 0.558 0.083 F019900500046 4.43 55.8 0.495 0.062 F019900500047 4.43 61.0 0.328 0.062 F019900500048 4.43 66.2 0.348 0.062 F019900500049 4.43 72.5 0.325 0.016 F019900500050 4.43 77.7 0.345 0.016 F019900500051 4.43 84.1 0.385 0.016 F019900500052 4.43 88.2 0.280 0.083 F019900500053 4.43 92.4 0.362 0.016 F019900500054 4.43 98.6 0.216 0.062 F019900500055 4.43 108.1 0.213 0.016 F019900500056 4.43 119.6 0.190 0.062 F019900500057 4.43 146.8 0.142 0.062 F019900500058 7.66 17.2 0.222 0.078 F019900500059 7.66 23.4 0.258 0.041 F019900500060 7.66 28.8 0.092 0.026 F019900500061 7.66 35.0 0.056 0.021 F019900500062 7.66 41.2 0.051 0.016 F019900500063 7.66 47.5 0.087 0.026 F019900500064 7.66 52.7 0.062 0.003 F019900500065 7.66 57.8 0.093 0.021 F019900500066 7.66 63.1 0.062 0.016 F019900500067 7.66 69.3 0.088 0.016 F019900500068 7.66 74.5 0.067 0.016 F019900500069 7.66 79.7 0.057 0.003 F019900500070 7.66 84.9 0.036 0.016 F019900500071 7.66 90.1 0.052 0.021 F019900500072 7.66 95.3 0.047 0.021 F019900500073 7.66 99.5 0.026 0.021 F019900500074 7.66 109.8 0.052 0.026 F019900500075 7.66 119.2 0.068 0.031 F019900500076 7.66 136.8 0.058 0.031 F019900500077 7.66 146.2 0.017 0.016 F019900500078 9.64 17.8 1.013 0.123 F019900500079 9.64 24.0 1.384 0.103 F019900500080 9.64 30.2 1.055 0.082 F019900500081 9.64 36.5 0.726 0.103 F019900500082 9.64 41.7 0.767 0.062 F019900500083 9.64 48.0 0.541 0.082 F019900500084 9.64 53.2 0.418 0.082 F019900500085 9.64 59.4 0.418 0.082 F019900500086 9.64 64.6 0.295 0.082 F019900500087 9.64 69.8 0.275 0.062 F019900500088 9.64 76.0 0.213 0.082 F019900500089 9.64 81.2 0.234 0.010 F019900500090 9.64 86.4 0.173 0.082 F019900500091 9.64 91.6 0.193 0.010 F019900500092 9.64 96.8 0.297 0.010 F019900500093 9.64 103.1 0.235 0.103 F019900500094 9.64 111.4 0.277 0.082 F019900500095 9.64 121.8 0.257 0.082 F019900500096 9.64 129.0 0.339 0.082 F019900500097 9.64 138.4 0.134 0.082 F019900500098 9.64 147.8 0.072 0.010 F019900500099 12.71 18.9 4.464 0.263 F019900500100 12.71 25.2 2.834 0.316 F019900500101 12.71 31.5 2.256 0.158 F019900500102 12.71 36.7 1.258 0.158 F019900500103 12.71 43.0 0.943 0.158 F019900500104 12.71 49.2 0.997 0.158 F019900500105 12.71 55.5 0.682 0.158 F019900500106 12.71 60.7 0.788 0.158 F019900500107 12.71 65.9 0.473 0.025 F019900500108 12.71 73.2 0.474 0.158 F019900500109 12.71 77.3 0.316 0.025 F019900500110 12.71 83.6 0.265 0.025 F019900500111 12.71 93.9 0.213 0.025 F019900500112 12.71 100.2 0.214 0.025 F019900500113 12.71 104.3 0.267 0.025 F019900500114 12.71 114.7 0.269 0.025 F019900500115 12.71 123.0 0.322 0.025 F019900500116 12.71 132.4 0.218 0.158 F019900500117 12.71 150.1 0.063 0.158 F019900500118 ENDDATA 102 0 F019900500119 ENDSUBENT 118 0 F019900599999 ENDENTRY 5 0 F019999999999